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Table 2.

Properties of Haro 11.

Property Unit Value Reference
Other name ... ESO 350-IG38 1
RA (J2000) h:m:s 00:36:52.7 1
Dec (J2000) d:m:s –33:33:17 1
Vsys(optical) km s−1 6194 ± 5.1 2
Redshift ... 0.0206467 2
Distance Mpc 87.2 ± 6.1 3
Scale pc/arcsec−1 ∼420 3
M* 109M 2.6 ± 0.8 4
Vsys (CO) km s−1 6051.3 ± 2.1 4
CO(1–0) flux Jy km s−1 3.3 ± 0.1 4
[C I] flux Jy km s−1 7.4 ± 0.3 4
MH2(CO) 109M 3.8 4
MH2([CI]) 108M 2.1-5.3 4
MHI 108M 5.1 5
SFRHα+TIR M yr−1 6
SFRHα(HST) M yr−1 24.0 7
SFRTIR M yr−1 28.6 8
SFRHα M yr−1 25.1 ± 0.4 4
Size kpc2 12.5 4
σv km s−1 17.2 4
Pturb 106 K cm−3 3.4 4
αvir ... 0.17 4

Notes. The Kroupa (2001) IMF is used to derive the stellar mass and SFR in this work. We assume the CO-H2 conversion factor αCO as 60 M (K km s−1 pc−2)−1, with a range of 10−110 M (K km s−1 pc−2)−1. We used the Python packages Statmorph to estimate the radius R80 containing 80% flux in r band, and then calculated the size of Haro 11. The CO(1–0) velocity dispersion σv, internal turbulent pressure Pturb and the viral parameter αvir are shown as the median values with one-sigma ranges. We also used the [C I] luminosity to derive the molecular gas based on the calibration in Madden et al. (2020) at metallicities of 0.25 Z and 0.1 Z, respectively, with a systemic uncertainty of 0.3 dex.

References. (1) Östlin et al. (2015); (2) Menacho et al. (2021); (3) NED; (4) this work; (5) Pardy et al. (2016); (6) Rémy-Ruyer et al. (2015); (7) Hayes et al. (2007); (8) Madden et al. (2013).

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